Introduction to Statics

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Presentation transcript:

Introduction to Statics B C D E F G H A P O N M L K J I Statics is the branch of mechanics concerned with the analysis of loads (forces, torque/moment) on physical systems in static equilibrium which is when a system is either at rest, or its center of mass moves at constant velocity.

DISCLAIMER & USAGE The content of this presentation is for informational purposes only and is intended for students attending Louisiana Tech University only. The authors of this information do not make any claims as to the validity or accuracy of the information or methods presented. Any procedures demonstrated here are potentially dangerous and could result in damage and injury. Louisiana Tech University, its officers, employees, agents and volunteers, are not liable or responsible for any injuries, illness, damage or losses which may result from your using the materials or ideas, or from your performing the experiments or procedures depicted in this presentation. The Living with the Lab logos should remain attached to each slide, and the work should be attributed to Louisiana Tech University. If you do not agree, then please do not view this content. boosting application-focused learning through student ownership of learning platforms

Units of Measure physical quantity dimension SI system U.S. Customary Most units of measure can be broken down into the basic units of length (L), mass (M) and time (t). physical quantity dimension SI system U.S. Customary system length 𝐿 𝑚 𝑜𝑟 𝑚𝑚 1𝑚= 1,000𝑚𝑚 𝑖𝑛 𝑜𝑟 𝑓𝑡 12𝑖𝑛=1𝑓𝑡 area 𝐿 2 𝑚2 𝑜𝑟 𝑚𝑚2 1 𝑚 2 = 1,000 𝑚𝑚 2 =1,000,000 𝑚𝑚 2 𝑖𝑛2 𝑜𝑟 𝑓𝑡2 1 𝑓𝑡 2 = (12 𝑖𝑛) 2 =144 𝑖𝑛 2 volume 𝐿 3 𝑚3 𝑜𝑟 𝑚𝑚3 1 𝑚 3 = (1,000𝑚𝑚) 3 = 10 9 𝑚𝑚 3 𝑖𝑛3 𝑜𝑟 𝑓𝑡3 1 𝑓𝑡 3 = (12 𝑖𝑛) 3 =1728 𝑖𝑛 3 1 𝑦𝑑 3 = (3𝑓𝑡) 3 =27 𝑓𝑡 3

Units of Measure physical quantity dimension SI system U.S. Customary force 𝐹=𝑚∙𝑎 𝑀∙𝐿 𝑡 2 𝑁= 𝑘𝑔∙𝑚 𝑠 2 𝑘𝑁=1,000𝑁 𝑙𝑏 𝑙𝑏𝑓 1𝑘𝑖𝑝=1,000𝑙𝑏 pressure or stress = 𝑓𝑜𝑟𝑐𝑒 𝑎𝑟𝑒𝑎 𝑀∙𝐿 𝑡 2 ∙ 1 𝐿 2 = 𝑀 𝐿∙ 𝑡 2 𝑁 𝑚 2 =𝑃𝑎 𝑘𝑃𝑎=1,000𝑃𝑎 M𝑃𝑎=1,000,000𝑃𝑎 𝑙𝑏 𝑖𝑛 2 =𝑝𝑠𝑖 energy =𝑓𝑜𝑟𝑐𝑒∙𝑑𝑖𝑠𝑡𝑎𝑛𝑐𝑒 𝑀∙𝐿 𝑡 2 ∙𝐿 = 𝑀∙ 𝐿 2 𝑡 2 𝑁∙𝑚=𝐽 (𝐽𝑜𝑢𝑙𝑒) 𝑓𝑡∙𝑙𝑏 power = 𝑒𝑛𝑒𝑟𝑔𝑦 𝑡𝑖𝑚𝑒 𝑀∙ 𝐿 2 𝑡 2 ∙ 1 𝑡 = 𝑀∙ 𝐿 2 𝑡 3 𝑁∙𝑚 𝑠 = 𝐽 𝑠 =𝑊 (𝑊𝑎𝑡𝑡) 𝑓𝑡∙𝑙𝑏 𝑠 550 𝑓𝑡∙𝑙𝑏 𝑠 =ℎ𝑝 L = length M = mass t=time

Three Characteristics of Forces q 𝐹 x y denotes a vector Magnitude (F) how hard you are pushing or pulling graphically represented by the length of the arrow Direction (q) usually defined by an angle measured relative to a coordinate system Point of Application

Breaking a Force into x and y Components Recall trigonometric functions: q 𝐹 x y sin 𝜃 = 𝑜𝑝𝑝𝑜𝑠𝑖𝑡𝑒 ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑢𝑠𝑒 cos 𝜃 = 𝑎𝑑𝑗𝑎𝑐𝑒𝑛𝑡 ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑢𝑠𝑒 𝐹 𝑦 𝐹 𝑦 α sin 𝜃 = 𝐹 𝑦 𝐹 cos 𝜃 = 𝐹 𝑥 𝐹 𝐹 𝑥 𝐹 𝑦 =𝐹∙ sin 𝜃 𝐹 𝑥 =𝐹∙ cos 𝜃 How will the expressions change for 𝐹 𝑥 and 𝐹 𝑦 if you were given α instead of θ?

Resultants 𝑅 𝐹 2 (moved) 𝐹 2 𝐹 1 How can we find the net effect of two or more forces that act on a body? 𝑦 𝑅 𝐹 2 (moved) 𝐹 2 𝐹 1 Head to Tail 𝜃 𝑥 Point of Application Geometric Solution: Arrange applied forces head to tail Draw a vector starting at the tail of the first vector to the head of the last vector The new vector is the resultant

Resultants 𝑅 𝐹 2 𝐹 1 𝑅 𝑥 =Σ 𝐹 𝑥 𝑅 𝑦 =Σ 𝐹 𝑦 Generally… 𝑅 𝑥 =Σ 𝐹 𝑥 𝑅 𝑦 =Σ 𝐹 𝑦 Generally… How can we find the net effect of two or more forces that act on a body? 𝑦 Algebraic Solution: To obtain the components of the resultant force, sum the corresponding components of each force. 𝑅 𝑅 𝑦 𝐹 2𝑦 𝐹 2 𝑅 𝑥 = 𝐹 1𝑥 + 𝐹 2𝑥 = 𝐹 1 cos 𝜃 1 + 𝐹 2 cos 𝜃 2 𝐹 2𝑦 𝐹 1 𝑅 𝑦 = 𝐹 1𝑦 + 𝐹 2𝑦 = 𝐹 1 sin 𝜃 1 + 𝐹 2 sin 𝜃 2 𝐹 1𝑦 𝜃 To find the resultant, R, of the Rx and Ry components, use Pythagorean Theorem 𝜃 2 𝜃 1 𝑥 𝐹 2𝑥 𝑅 𝑥 𝐹 2𝑥 𝐹 1𝑥 𝑅= 𝑅 𝑥 2 + 𝑅 𝑦 2 To find the angle of the resultant, use the tangent function 𝜃= 𝑡𝑎𝑛 −1 𝑅 𝑦 𝑅 𝑥

Class Problem: Two ants are hitched to a beetle and pull with the forces shown: Find the x and y components of the force exerted by ant 1. Find the x and y components of the force exerted by ant 2. Find the x component of the resultant force of the ants. Find the y component of the resultant force of the ants. Find the resultant force of the ants. What angle does the resultant force make with the x-axis? 𝑦 Ant 1 = 0.014715𝑁 Solution: a. =0.01274𝑁 𝐹 1𝑥 = 𝐹 1 cos 30° =0.014715𝑁∙cos⁡(30°) 30° 𝑥 =0.00736𝑁 𝐹 1𝑦 = 𝐹 1 sin 30° =0.014715𝑁∙sin⁡(30°) 50° Beetle b. =0.01261𝑁 𝐹 2𝑥 = 𝐹 2 cos 50° =0.01962𝑁∙cos⁡(50°) =−0.01503𝑁 𝐹 2𝑦 = 𝐹 2 sin 50° =0.01962𝑁∙sin⁡(50°) Ant 2 = 0.01962𝑁 Negative since the force acts in the –y direction. You also know the result should be negative because sin⁡(50°) in QIV is negative. When accounting for the sign of a force, it is most intuitive to simply look at the force diagram and set forces to + or – based on their coordinate direction.

Solution: d. =0.02535𝑁 𝐹 1 =0.014715𝑁 𝑅 𝑥 = 𝐹 1𝑥 + 𝐹 2𝑥 =0.01274𝑁+0.01261𝑁 𝐹 1𝑥 =0.01274𝑁 𝑦 𝑅 𝑦 = 𝐹 1𝑦 + 𝐹 2𝑦 =0.00736𝑁−0.01503𝑁 =−0.00767𝑁 𝐹 1𝑦 =0.00736𝑁 Ant 1 = 1.5g 𝑅= 𝑅 𝑥 2 + 𝑅 𝑦 2 = (0.02535𝑁 ) 2 + (−0.00767𝑁 ) 2 e. =0.02648𝑁 𝜃= tan −1 𝑅 𝑦 𝑅 𝑥 = tan −1 −0.00767𝑁 0.02535𝑁 f. =−16.83° 30° −16.83° 𝑥 50° Beetle Ant 2 = 2g 𝐹 2 =0.01960𝑁 𝐹 2𝑥 =0.01261𝑁 𝐹 2𝑦 =−0.01503𝑁

Class Problem: Three water skiers are pulled by a boat as shown Class Problem: Three water skiers are pulled by a boat as shown. Determine The resultant force of the water skiers. The direction of the resultant measured counterclockwise from the positive x-axis. Draw the resultant force and label the computed angle on an x-y coordinate system. 𝐹 1𝑥 =−140𝑙𝑏∙𝑠𝑖𝑛⁡(40°) =−89.99𝑙𝑏 𝐹 2𝑥 =−100𝑙𝑏∙𝑐𝑜𝑠⁡(15°) =−96.59𝑙𝑏 𝐹 1𝑦 =140𝑙𝑏∙𝑐𝑜𝑠⁡(40°) =107.25𝑙𝑏 𝐹 2𝑦 =100𝑙𝑏∙𝑠𝑖𝑛⁡(15°) =25.88𝑙𝑏 𝐹 3𝑥 =−200𝑙𝑏∙𝑐𝑜𝑠⁡(65°) =−84.52𝑙𝑏 𝐹 3𝑦 =−200𝑙𝑏∙𝑠𝑖𝑛⁡(65°) =−181.26𝑙𝑏 𝛽=190.07° =−89.99𝑙𝑏−96.59𝑙𝑏−84.52𝑙𝑏 =−271.1𝑙𝑏 𝑅 𝑥 = 𝐹 1𝑥 + 𝐹 2𝑥 + 𝐹 3𝑥 =107.25𝑙𝑏+25.88𝑙𝑏−181.26𝑙𝑏 =−48.13𝑙𝑏 𝑅 𝑦 = 𝐹 1𝑦 + 𝐹 2𝑦 + 𝐹 3𝑦 𝑅= 𝑅 𝑥 2 + 𝑅 𝑦 2 = −271.1𝑙𝑏 2 + −48.13𝑙𝑏 2 =275.34𝑙𝑏 𝛽= tan −1 −48.13𝑙𝑏 −271.1𝑙𝑏 =10.07° in QIII, so 190.07° measured CCW from positive x-axis